WO2012036138A1 - Procédé et dispositif d'analyse - Google Patents

Procédé et dispositif d'analyse Download PDF

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Publication number
WO2012036138A1
WO2012036138A1 PCT/JP2011/070774 JP2011070774W WO2012036138A1 WO 2012036138 A1 WO2012036138 A1 WO 2012036138A1 JP 2011070774 W JP2011070774 W JP 2011070774W WO 2012036138 A1 WO2012036138 A1 WO 2012036138A1
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Prior art keywords
plasma
analysis
emission intensity
substance
electromagnetic wave
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PCT/JP2011/070774
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English (en)
Japanese (ja)
Inventor
池田　裕二
寉岡亮治
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イマジニアリング株式会社
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Application filed by イマジニアリング株式会社 filed Critical イマジニアリング株式会社
Priority to EP11825140.4A priority Critical patent/EP2618132A4/fr
Priority to JP2012534004A priority patent/JP5906501B2/ja
Publication of WO2012036138A1 publication Critical patent/WO2012036138A1/fr
Priority to US13/839,560 priority patent/US8879061B2/en

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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/02—Details
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28—Investigating the spectrum
    • G01J3/443—Emission spectrometry
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/66—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light electrically excited, e.g. electroluminescence
    • G01N21/68—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light electrically excited, e.g. electroluminescence using high frequency electric fields
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/71—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited
    • G01N21/718—Laser microanalysis, i.e. with formation of sample plasma

Definitions

  • the present invention relates to an analysis apparatus and an analysis method for analyzing a substance to be analyzed by analyzing light emitted from plasma.
  • Patent Document 1 discloses this type of analyzer.
  • Patent Document 1 describes an elemental analyzer using laser-induced breakdown (spectrum).
  • this elemental analyzer pulse laser light emitted from a laser oscillator is condensed on the sample surface, and a part of the sample surface is turned into plasma.
  • the constituent elements on the sample surface become atoms in an excited state.
  • the atom in the excited state emits fluorescence when transitioning to the lower level.
  • the emitted fluorescence enters the fluorescence detector via the optical fiber.
  • the fluorescence detector converts information about the wavelength of fluorescence and the intensity of this wavelength into an electrical signal.
  • the computer for measurement control performs elemental analysis based on the converted electrical signal.
  • the analysis target substance is converted into plasma using only the pulsed laser beam, so that the time during which plasma is formed is short. For this reason, the integrated value of the emission intensity of the light emitted from the plasma does not become so large, and it is difficult to perform highly accurate analysis. Moreover, in order to improve the analysis accuracy, it was necessary to use a high-performance spectrometer.
  • the present invention has been made in view of the above points, and an object of the present invention is to improve analysis accuracy in an analyzer that analyzes a substance to be analyzed by analyzing plasma light emitted from plasma.
  • energy is instantaneously applied to a substance to be analyzed to generate an initial plasma in which the substance to be analyzed is in a plasma state, and the initial plasma is irradiated with an electromagnetic wave for a predetermined time to change the plasma state.
  • An analyzer comprising: plasma generating means for maintaining; and light analyzing means for analyzing the substance to be analyzed using a time integral value of light emission intensity of light emitted from the electromagnetic wave plasma maintained by the electromagnetic waves.
  • the plasma is maintained until immediately after the irradiation of the electromagnetic waves is stopped. Since the irradiation time of the electromagnetic wave can be easily controlled, the existence time of the electromagnetic wave plasma can be easily controlled.
  • the time integral value of the emission intensity of the electromagnetic wave plasma whose existence time can be controlled is used for the analysis of the analysis target substance.
  • the time integral value of the light emission intensity of the light emitted from the electromagnetic plasma is larger than the time integral value of the light emission intensity of the light emitted from the initial plasma.
  • the plasma generating means is controlled.
  • the light emitted from the electromagnetic wave plasma includes a light emission of a molecule, and is irradiated from the electromagnetic wave irradiation means so that the peak of the light emission intensity of the molecule can be detected.
  • the energy per unit time of the electromagnetic wave is adjusted.
  • the energy per unit time of the electromagnetic wave irradiated from the electromagnetic wave irradiation means is adjusted so that the plasma light generated by the electromagnetic wave plasma includes the emission of the molecule and the peak of the emission intensity of the molecule can be detected. Yes.
  • the substance to be analyzed is a particulate substance or a gaseous substance contained in a fluid
  • the optical analysis means includes the electromagnetic wave
  • the substance to be analyzed is analyzed by using the time integral value of the light emission intensity taken from the area larger than the initial plasma formation area in the plasma formation area.
  • the substance to be analyzed is analyzed using the time integral value of the light emission intensity taken from the region larger than the initial plasma formation region in the electromagnetic plasma formation region.
  • the substance to be analyzed is a particulate substance or a gaseous substance contained in the fluid
  • the substance amount of the specific substance may be uneven depending on the location.
  • a component in a small region is analyzed, a difference occurs in the analysis result every time it is analyzed, and the reliability of the analysis result cannot be ensured. Therefore, it is conceivable to analyze components in a certain large area.
  • the plasma light emitted from the laser plasma is analyzed, the plasma formation region is small, so that components in a large region cannot be analyzed.
  • the fourth invention since the plasma is expanded by the electromagnetic wave, it is possible to analyze light taken from a region larger than a region where the initial plasma is formed. Therefore, the substance to be analyzed is analyzed using the time integration value of the light emission intensity taken from the area larger than the formation area of the initial plasma.
  • the energy per unit time of the electromagnetic wave irradiated by the plasma generating means and the continuous irradiation of the electromagnetic wave according to the phase state of the substance to be analyzed At least one of time is controlled.
  • At least one of the energy per unit time of the electromagnetic wave and the irradiation duration time of the electromagnetic wave is controlled according to the phase state of the substance to be analyzed.
  • the plasma generation means repeats generation and extinction of plasma at a predetermined operation cycle, and the light detection means is controlled by the plasma generation means. Every time plasma is generated, the analysis target substance is analyzed using the time integral value of the emission intensity of light emitted from the electromagnetic wave plasma, and the electromagnetic wave irradiated by the plasma generating means is shortened as the operation period is shortened. Increase the energy per unit time.
  • the shorter the operation cycle of the plasma generation means the shorter the operation cycle of the optical analysis means operating correspondingly. That is, the time responsiveness of the analyzer is increased. The higher the time response of the analyzer, the higher the energy per unit time of the electromagnetic wave.
  • the shorter the operation cycle of the plasma generating means the shorter the period during which the electromagnetic wave plasma is formed. For this reason, if the energy per unit time of the electromagnetic wave is constant, the time integral value of the emission intensity of the electromagnetic wave plasma becomes smaller as the operation cycle of the plasma generating means is shortened.
  • the shorter the operation cycle of the plasma generation means the shorter the operation cycle of the plasma generation means, so that the time integral value of the emission intensity of the electromagnetic wave plasma becomes a large value even if the operation cycle of the plasma generation means is shortened.
  • the energy per unit time is increased.
  • the plasma generating means is provided in a space in which initial plasma is generated during a plasma maintenance period in which the plasma generating means maintains the plasma. Electromagnetic waves are radiated from a radiating antenna in a continuous wave.
  • the plasma generating means radiates the electromagnetic wave in a continuous wave (CW) during the plasma maintenance period in which the plasma is maintained by the energy of the electromagnetic wave.
  • CW continuous wave
  • the energy of the electromagnetic wave is stably given without pulsating like the electromagnetic wave pulse. Therefore, it is possible to suppress the generation of shock waves due to electromagnetic waves in the plasma region during the plasma maintenance period.
  • the substance to be analyzed is moved to the electromagnetic wave plasma region during the plasma maintenance period.
  • the plasma generating means radiates an electromagnetic wave from the radiation antenna in response to a pulse signal having a constant voltage value
  • the optical analysis means is the plasma sustaining period.
  • an analysis period is set within a certain period of emission intensity in which the variation amount of the emission intensity of the plasma light is a predetermined value or less, and the analysis target substance is analyzed based on the emission intensity of the plasma light in the analysis period.
  • the substance to be analyzed is a powdery substance
  • the plasma generation unit is configured to output an electromagnetic wave during the plasma maintenance period. The value is set so that the target substance does not scatter.
  • the maximum value of the plasma emission intensity in the plasma sustain period is larger than the maximum value of the emission intensity of the initial plasma.
  • the output of the electromagnetic wave during the plasma maintenance period is set.
  • the optical analysis means analyzes the plasma light during the plasma maintenance period and determines a mixing ratio of components contained in the analysis target substance. To detect.
  • the optical analysis means analyzes the plasma light during the plasma maintenance period and detects the temperature of the gas in the electromagnetic wave plasma region.
  • an initial plasma is generated in which energy is instantaneously applied to a substance to be analyzed to bring the substance to be analyzed into a plasma state, and the initial plasma is irradiated with an electromagnetic wave for a predetermined time to change the plasma state.
  • An analysis method comprising: a plasma generation step to be maintained; and an optical analysis step to analyze the substance to be analyzed using a time integral value of light emission intensity of light emitted from the electromagnetic wave plasma maintained by the electromagnetic wave.
  • the analysis target substance is analyzed using the time integral value of the emission intensity of the electromagnetic wave plasma capable of controlling the existence time.
  • the electromagnetic wave plasma can be maintained for a longer time than when plasma is formed using only pulsed laser light, for example. Therefore, since a large value can be acquired as the time integral value of the emission intensity, it is possible to perform a highly accurate analysis without using a high-performance spectrometer.
  • the plasma light generated by the electromagnetic wave plasma includes the light emission of the molecule, and the peak of the light emission intensity of the molecule can be detected, so that an analyzer capable of analyzing the molecule can be realized. it can.
  • the analysis target substance is analyzed using the time integral value of the light emission intensity taken from the area larger than the formation area of the initial plasma. Therefore, when the analysis target substance is a particulate substance contained in a fluid or a gas component, an analyzer that can analyze a component in a large region can be realized. Then, when the analysis target substance is a particulate substance or a gas component contained in the fluid, a highly reliable analysis can be performed.
  • the shorter the operation cycle of the plasma generation means the shorter the operation cycle of the plasma generation means, so that the time integral value of the emission intensity of the electromagnetic wave plasma becomes a large value even if the operation cycle of the plasma generation means is shortened.
  • the energy per unit time is increased. Therefore, even if the operation cycle of the plasma generating means is shortened, that is, the time responsiveness of the analyzer is increased, high-precision analysis can be performed.
  • the seventh aspect since the energy of electromagnetic waves is stably given to the plasma region during the plasma maintenance period, it is possible to suppress the generation of shock waves due to the electromagnetic waves.
  • the analysis period in which the optical analysis means performs analysis exists in the plasma maintenance period. Therefore, when a powdery substance is used as an analysis target substance, the analysis target substance in the plasma region can be prevented from scattering during the analysis period.
  • the substance to be analyzed in the plasma region can be analyzed with almost no movement of the substance.
  • FIG. 1 is a schematic configuration diagram of the analyzer according to the first embodiment.
  • FIG. 2 is a diagram for explaining the plasma generation maintaining operation of the first embodiment.
  • FIG. 3 is a graph showing time-series changes in the emission intensity of light emitted from the plasma generated by the plasma generation apparatus of the first embodiment.
  • FIG. 4 is a spectrum diagram showing a time integration value of the emission intensity corresponding to the wavelength with respect to light emitted from the plasma generated by the plasma generation apparatus of the first embodiment.
  • FIG. 5 is a schematic configuration diagram of the analyzer according to the second embodiment.
  • FIG. 6 is a schematic configuration diagram of the plasma generation apparatus according to the second embodiment.
  • FIG. 7 is a schematic configuration diagram of the analyzer according to the third embodiment.
  • FIG. 8 is a time chart illustrating the time relationship between the pulse oscillation signal and the electromagnetic wave drive signal according to the third embodiment.
  • FIG. 9 is a graph showing time-series changes in the emission intensity of light emitted from plasma generated by the plasma generation apparatus of the third embodiment.
  • FIG. 10 is a schematic configuration diagram of the analyzer according to the fourth embodiment.
  • Embodiment 1 is essentially preferable examples, and are not intended to limit the scope of the present invention, its application, or its use.
  • the analyzer 10 includes a plasma generator 11, a cavity 12, an optical analyzer 13, and a controller 14.
  • the control device 14 controls the plasma generation device 11 and the optical analysis device 13.
  • the analyzer 10 of this Embodiment 1 is a substance which can be made into a plasma state with the plasma production
  • the plasma generator 11 includes a laser light source 21, a condensing optical system 22, a microwave oscillator 23, microwave transmission paths 24 to 27, an antenna 28, and a pulse power source 29.
  • the plasma generation device 11 instantaneously applies energy to the analysis target substance 15 to generate an initial plasma in which the analysis target substance 15 is brought into a plasma state, and irradiates the initial plasma with an electromagnetic wave for a predetermined time to change the plasma state.
  • the plasma generating means to maintain is comprised.
  • the laser light source 21 and the condensing optical system 22 constitute initial plasma generating means for applying energy to the analysis target substance 15 to change the analysis target substance 15 into a plasma state.
  • the microwave oscillator 23, the microwave transmission paths 24 to 27, the antenna 28, and the pulse power source 29 are plasmas that maintain the plasma state by irradiating the initial plasma generated by the initial plasma generating means with electromagnetic waves for a predetermined time. It constitutes a maintenance means.
  • the laser light source 21 oscillates a laser beam for bringing the analysis target substance 15 into a plasma state.
  • the laser light oscillated from the laser light source 21 passes through the condensing optical system 22 and is condensed at the focal point of the condensing optical system 22.
  • the focal point of the condensing optical system 22 is located in the cavity 12.
  • the laser light source 21 for example, an Nd: YAG laser light source is used.
  • a convex lens is used for the condensing optical system 22.
  • the plasma generation device 11 is configured such that the energy density of the laser beam condensed at the focal point of the condensing optical system 22 is equal to or higher than the breakdown threshold of the analysis target substance 15. That is, the output of the laser beam is set to a value higher than that necessary for the analysis target substance 15 present at the focal point to be converted into plasma.
  • the microwave oscillator 23 is connected to the antenna 28 via microwave transmission paths 24 to 27.
  • the microwave transmission paths 24 to 27 include a waveguide 24 connected to the microwave oscillator 23, an isolator 25 connected to the waveguide 24, a coaxial waveguide converter 26 connected to the isolator 25, A coaxial cable 27 is connected to the coaxial waveguide converter 26.
  • the microwave oscillator 23 is connected to a pulse power supply 29. The microwave oscillator 23 oscillates a microwave when supplied with power from the pulse power supply 29.
  • the antenna 28 is connected to the coaxial cable 27.
  • the tip of the antenna 28 is directed to the focal position of the condensing optical system 22.
  • the microwave oscillated from the microwave oscillator 23 is irradiated from the antenna 28 toward the focal position of the condensing optical system 22 through the microwave transmission paths 24 to 27.
  • microwave oscillator 23 for example, a magnetron that oscillates a microwave of 2.45 GHz is used.
  • antenna 28 for example, a 3/4 wavelength monopole antenna is used as an antenna having a sufficient gain with respect to the microwave oscillated from the microwave oscillator 23.
  • pulse power supply 29 for example, an inverter type power supply device is used.
  • the cavity 12 is a substantially cylindrical container having a microwave resonance structure, and prevents the microwave from leaking to the outside.
  • the cavity 12 is provided with a support member (not shown) that supports the analysis target substance 15.
  • the cavity 12 is provided with an introduction window for introducing laser light oscillated from the laser light source 21. Laser light oscillated from the laser light source 21 is incident on the cavity 12.
  • the substance to be analyzed 15 is brought into a plasma state by the laser light.
  • the microwave is irradiated from the antenna 28 to the analysis target substance 15 in the plasma state.
  • the plasma generation device 11 performs a plasma generation maintenance operation for maintaining the plasma state by setting the analyte 15 to a plasma state in accordance with an instruction from the control device 14.
  • the pulse power supply 29 receives the start signal output from the control device 14, the supply of power to the microwave oscillator 23 is started.
  • the microwave oscillator 23 starts the oscillation of the microwave, and the analysis target substance 15 in the cavity 12 is irradiated with the microwave from the antenna 28.
  • the microwaves resonate to form a standing wave.
  • the vicinity of the laser irradiation surface of the analysis target substance 15 becomes an antinode of a standing wave and becomes a strong electric field region.
  • the laser light source 21 receives the oscillation signal output from the control device 14, it oscillates only one pulsed laser beam.
  • the laser light is oscillated immediately after the start of microwave irradiation.
  • the laser light oscillated from the laser light source 21 is condensed on the surface of the analysis target substance 15 by the condensing optical system 22.
  • the analysis target substance 15 is instantaneously given a high density energy.
  • the energy density in the laser light irradiation region increases and exceeds the breakdown threshold of the analysis target substance 15. Then, as shown in FIG. 2, the substance in the laser light irradiation region is ionized to be in a plasma state. That is, plasma is generated using the analysis target substance 15 as a raw material.
  • plasma generated by laser light is referred to as “laser plasma”.
  • Laser plasma corresponds to initial plasma.
  • microwave plasma corresponds to electromagnetic plasma.
  • the microwave oscillator 23 stops the oscillation of the microwave.
  • the microwave oscillator 23 is stopped after the laser light is oscillated.
  • the microwave irradiation is stopped, for example, 5 seconds after the end of the laser light oscillation. Then, recombination of electrons occurs and the microwave plasma disappears.
  • the pulse power supply 29 repeatedly supplies a pulse wave (or burst wave) to the microwave oscillator 23 during the period from the reception of the start signal to the reception of the stop signal.
  • the pulse power supply 29 supplies power to the microwave oscillator 23 at a predetermined duty ratio (on / off duty ratio).
  • the microwave oscillator 23 repeats the oscillation and stoppage of the microwave at a predetermined duty ratio.
  • the microwave plasma does not become a thermal plasma and is maintained as a non-equilibrium plasma.
  • the start of microwave oscillation is the time when the first pulse wave is received
  • the end of the microwave oscillation is the time when the last pulse wave is received.
  • the period from receiving the start signal to receiving the stop signal is a microwave irradiation period. Further, the energy per unit time of the microwave is kept constant without being adjusted over the microwave irradiation period.
  • the microwave oscillation start timing is before the laser beam oscillation, but may be after the laser beam oscillation as long as the laser plasma is extinguished.
  • the peak of the emission intensity due to the laser plasma is first seen instantaneously as shown in FIG.
  • the emission intensity decreases to a minimum value near zero. Then, after the emission intensity reaches the minimum value, the emission intensity is increased again by the microwave plasma, and the emission intensity is kept at a certain level until the disappearance of the microwave plasma is started.
  • laser plasma plasma up to a minimum value immediately after the peak of emission intensity by laser plasma
  • microwave plasma plasma after the minimum value
  • the plasma generating apparatus 11 is configured so that the maximum value of the emission intensity of laser plasma is larger than that of microwave plasma.
  • the output of the laser light source 21 and the output of the microwave oscillator 23 are set so that the energy density in the plasma is higher in the microwave plasma than in the laser plasma.
  • the optical analyzer 13 analyzes only the plasma light emitted from the microwave plasma during the plasma generation maintaining operation.
  • the optical analysis device 13 constitutes an optical analysis means for analyzing the analysis target substance 15 by using a time integral value of light emission intensity of light emitted from electromagnetic wave plasma maintained by electromagnetic waves.
  • the optical analyzer 13 includes a beam sampler 30, a first power meter 31A, a second power meter 31B, an optical element 32, an optical fiber 33, a spectrometer 34, a photodetector 35, and a signal processing device 36.
  • the beam sampler 30 is disposed between the laser light emitting portion of the laser light source 21 and the condensing optical system 22.
  • the beam sampler 30 separates a part of the laser light oscillated from the laser light source 21.
  • the first power meter 31A receives the light separated by the beam sampler 30.
  • the output signal of the first power meter 31A is input to the signal processing device 36.
  • the second power meter 31 ⁇ / b> B is disposed on the opposite side of the cavity 12 with respect to the laser light source 21 and receives the laser light that has passed through the cavity 12.
  • the output signal of the second power meter 31B is input to the signal processing device 36.
  • the optical element 32 includes a lens that transmits light.
  • a condensing optical system is used as the optical element 32.
  • the optical element 32 is arranged so that its focal point is located in the formation region of the microwave plasma.
  • the spectroscope 34 is connected to the optical element 32 via the optical fiber 33.
  • the spectroscope 34 receives plasma light incident on the optical element 32.
  • the spectroscope 34 uses a diffraction grating or a prism to disperse the incident plasma light in different directions depending on the wavelength.
  • a shutter 37 is provided as a delimiting means. The shutter 37 is switched by the control device 14 between an open state in which light is allowed to enter the spectroscope 34 and a closed state in which light is not allowed to enter the spectroscope 34.
  • the control apparatus 14 may constitute an analysis time division unit.
  • the photodetector 35 is disposed so as to receive light in a predetermined wavelength band among the light dispersed by the spectroscope 34. In response to the command signal output from the control device 14, the photodetector 35 converts the received light in the wavelength band into an electrical signal for each wavelength and outputs the electrical signal.
  • a charge coupled device is used for the photodetector 35.
  • the electrical signal output from the photodetector 35 is input to the signal processing device 36.
  • the signal processing device 36 calculates a time integrated value of the emission intensity for each wavelength based on the electric signal output from the photodetector 35.
  • a time integral value (emission spectrum) of the emission intensity for each wavelength is obtained for the plasma light incident on the spectrometer 34 while the shutter 37 is in the open state.
  • the signal processing device 36 creates a graph showing the time integration value of the emission intensity for each wavelength as shown in FIG. Further, the signal processing device 36 identifies a component of the analysis target substance 15 by finding a wavelength component having a high emission intensity from the time integrated value of the emission intensity for each wavelength.
  • the signal processing device 36 detects the energy of the laser light oscillated from the laser light source 21 by using the output value of the first power meter 31A and the separation rate of the laser light by the beam sampler 30.
  • the signal processing device 36 detects the energy of the laser light that has passed through the cavity 12 using the output value of the second power meter 31B.
  • the signal processing device 36 detects the energy absorbed in the plasma from the difference between the energy of the laser light oscillated from the laser light source 21 and the energy of the laser light that has passed through the cavity 12.
  • the optical analyzer 13 performs an optical analysis operation for analyzing plasma light emitted from the plasma in accordance with instructions from the control device 14.
  • the optical analysis operation is performed in conjunction with the plasma generation maintaining operation. Further, in the plasma generation maintaining operation, the control device 14 controls the shutter 37 so as to be opened only during a period in which the microwave plasma is formed.
  • plasma light emitted from the microwave plasma is incident on the spectroscope 34 through the optical element 32 and the optical fiber 33 in order while the shutter 37 shown in FIG. 3 is open.
  • the incident plasma light is dispersed in different directions depending on the wavelength.
  • plasma light having a predetermined wavelength band reaches the photodetector 35.
  • the received plasma light in the wavelength band is converted into an electrical signal for each wavelength.
  • the signal processing device 36 the time integrated value of the light emission intensity is calculated for each wavelength based on the output signal of the photodetector 35.
  • the signal processing device 36 finds a wavelength component having a strong emission intensity from the time integrated value of the emission intensity for each wavelength, and identifies the component of the analysis target substance 15.
  • the signal processing device 36 may create a graph indicating the time integrated value of the emission intensity for each wavelength as shown in FIG. 4 and display the graph on the monitor of the signal processing device 36.
  • the user of the analysis apparatus 10 can identify atoms contained in the analysis target substance as a component analysis of the analysis target substance by viewing the spectrum diagram.
  • the analyzer 10 may calculate the content of the specified atom using a calibration curve.
  • the signal processing device 36 may correct the atomic content obtained from the emission spectrum using the detected value of the energy of the laser light oscillated from the laser light source 21.
  • the signal processing device 36 may correct the atomic content obtained from the emission spectrum by using the detected value of the energy absorbed in the plasma.
  • the analyzer 10 of this embodiment can perform not only the atom but the identification of the molecule
  • the energy density of the laser is too high, and most of the molecules contained in the target substance are decomposed into atoms. .
  • the light emission of the molecule is weak and the peak of the light emission of the molecule cannot be detected.
  • the energy per unit time of the microwave irradiated from the antenna 28 includes the emission of molecules (for example, OH radicals) in the light emitted from the microwave plasma, and the emission of the molecules.
  • the intensity is adjusted to a value below which a peak of intensity can be detected. Therefore, many molecules remain in the microwave plasma without being decomposed, and the peak of the emission intensity of the molecule can be detected from the emission spectrum detected by the analyzer 13. -Effect of Embodiment 1-
  • the analysis target substance 15 is analyzed using the time integral value of the emission intensity of the microwave plasma capable of controlling the existence time.
  • Microwave plasma can be maintained for a longer time than when plasma is formed using only pulsed laser light. Therefore, since a large value can be acquired as the time integral value of the emission intensity, it is possible to perform a highly accurate analysis without using a high-performance spectrometer.
  • the plasma light generated by the microwave plasma includes light emission of a molecule, and the peak of the light emission intensity of the molecule can be detected. Therefore, the analyzer 10 capable of analyzing the molecule is realized. Can do. —Modification 1 of Embodiment 1—
  • the analysis apparatus 10 of the first modification is an apparatus that analyzes a particulate substance or a gaseous substance contained in a fluid as an analysis target substance.
  • the optical analysis device 13 does not use the optical element 32 focused on the microwave plasma formation region, but emits light emitted from an analysis target region larger than the laser plasma formation region in the microwave plasma formation region.
  • An optical element 32 that can be captured is used.
  • the plasma light emitted from the analysis target region is taken into the spectroscope 34, and the time integral value of the emission intensity of the analysis target region is calculated by the analyzer 13, and the analysis target is calculated using the time integration value.
  • the constituents of the substance are analyzed.
  • the substance to be analyzed is analyzed using the time integral value of the light emission intensity taken from the region larger than the region where the laser plasma is formed. Therefore, it is possible to realize an analyzer capable of analyzing a large area when the analysis target substance is a particulate substance or a gaseous substance contained in the fluid. Then, when the analysis target substance is a particulate substance or a gaseous substance contained in the fluid, a highly reliable analysis can be performed.
  • the energy per unit time of the microwave oscillated from the microwave oscillator 23 is adjusted according to the phase state of the analysis target substance.
  • the analyzer 10 is provided with an input unit for inputting the phase state of the substance to be analyzed.
  • the user of the analyzer 10 operates the input unit according to the analysis target substance 15.
  • the maximum voltage of the pulse wave output from the pulse power supply 29 is set according to the output signal of the input unit.
  • the energy per unit time of the microwave oscillated from the microwave oscillator 23 becomes a value corresponding to the phase state of the substance to be analyzed.
  • the breakdown threshold is higher for solids than for gases. Accordingly, the solid energy is set to a larger value per unit time than the gas.
  • the duration of microwave irradiation oscillated from the microwave oscillator 23 may be adjusted according to the output signal of the input unit. Thereby, the irradiation duration of the microwave oscillated from the microwave oscillator 23 is adjusted according to the phase state of the substance to be analyzed. —Modification 3 of Embodiment 1
  • the analysis device 10 of the third modification example allows the user to set the analysis time interval. Further, the shorter the analysis time interval set by the user, the higher the energy per unit time of the microwave oscillated from the microwave oscillator 23 is adjusted.
  • the plasma generator 11 repeats the generation and extinction of plasma using the input analysis time interval as an operation cycle.
  • the optical analyzer 13 operates in conjunction with the plasma generator 11 and analyzes using the time integral value of the light emission intensity of light emitted from the microwave plasma each time plasma is generated by the plasma generator 11. Analyze the components of the target substance. As described above, the analysis apparatus 10 performs the optical analysis operation for analyzing the analysis target substance at the analysis time interval set by the user.
  • the energy per unit time of the microwave is increased as the analysis time interval is shortened so that the time integration value of the emission intensity of the microwave plasma becomes a large value even if the analysis time interval is shortened. Yes. Therefore, even if the analysis time interval is shortened, that is, even if the time responsiveness of the analyzer 10 is increased, a highly accurate analysis can be performed. ⁇ Embodiment 2 >>
  • Embodiment 2 differs from Embodiment 1 in the initial plasma generation means.
  • a discharge device for example, a spark plug
  • the plasma generation apparatus 11 includes a pulse voltage generator 51, a microwave oscillator 23, a mixer 52, a matching unit 53, and a spark plug 54.
  • the pulse voltage generator 51, the mixer 52, the matching device 53, and the spark plug 54 are integrated to form an ignition unit 58 (the description of the matching device 53 is omitted in FIG. 5). is doing).
  • the pulse voltage generator 51 is supplied with DC power from an external DC power supply 60. Upon receiving the discharge signal output from the control device 14, the pulse voltage generator 51 generates and outputs a high voltage pulse voltage.
  • the pulse voltage is an impulse voltage signal having a peak voltage of about 6 kV to 40 kV, for example.
  • the specifications of the pulse voltage may be set as appropriate so that dielectric breakdown occurs when a pulse voltage is applied to the spark plug 54.
  • the mixer 52 receives a pulse voltage from the pulse voltage generator 51 and a microwave from the microwave oscillator 23.
  • the mixer 52 generates and outputs a mixed signal obtained by mixing the pulse voltage and the microwave.
  • the mixed signal is transmitted to the spark plug 54 via the matching unit 53.
  • the matching unit 53 performs impedance matching of the microwave output from the mixer 52.
  • a discharge gap is formed between the discharge electrode 54a and the ground electrode 54b.
  • a discharge is generated and a microwave is emitted.
  • a small-scale discharge plasma (initial plasma) is formed by the discharge, and the discharge plasma absorbs microwave energy and expands.
  • the expanded plasma becomes microwave plasma.
  • the microwave is irradiated for a predetermined time.
  • the microwave oscillation start timing is before the spark discharge, but may be after the spark discharge as long as it is before the discharge plasma is extinguished.
  • the analysis target substance 15 is arranged in the discharge gap.
  • the analysis target substance 15 is supported by a support member (not shown).
  • the analysis device 10 of the third embodiment is a device that performs a component analysis of the analysis target substance 100 using a powdery substance as the analysis target substance 100.
  • the analyzer 10 is used for detecting impurities, for example.
  • the analysis apparatus 10 is installed with respect to a belt conveyor 101 that moves the analysis target substance 100.
  • the analysis device 10 includes a plasma generation device 111, a cavity 112, an optical analysis device 113, and a control device 114.
  • the cavity 112 is a container having a microwave resonance structure.
  • the cavity 112 is formed in a substantially cylindrical shape whose lower side is open.
  • the cavity 112 is configured by a mesh-like member.
  • the size of the mesh of the cavity 112 is set so that the microwave radiated from the radiation antenna 128 (described later) to the internal space of the cavity 112 does not leak to the outside.
  • a laser probe 123 and an antenna probe 126 are attached to the upper surface of the cavity 112. Further, the control device 114 controls the plasma generation device 111 and the optical analysis device 113. -Configuration of plasma generator-
  • the plasma generation device 111 constitutes plasma generation means for generating plasma in the space and maintaining the plasma by the energy of microwaves radiated from the radiation antenna 128.
  • the plasma generator 111 instantaneously applies energy to a substance in the space to generate an initial plasma in which the substance is put into a plasma state, and the initial plasma is irradiated with microwaves for a predetermined time to generate a plasma state. To maintain.
  • the plasma generation device 111 includes a laser oscillation device 115 and an electromagnetic wave emission device 116 as shown in FIG.
  • the laser oscillation device 115 includes a laser light source 121, an optical fiber 122, and a laser probe 123.
  • the electromagnetic wave radiation device 116 includes a microwave oscillator 124, a microwave transmission line 125, and an antenna probe 126.
  • the laser light source 121 When the laser light source 121 receives a laser oscillation signal from the control device 114, the laser light source 121 oscillates a laser beam for generating initial plasma.
  • the laser light source 121 is connected to a laser probe 123 via an optical fiber 122.
  • a condensing optical system 127 that condenses the laser light that has passed through the optical fiber 122 is provided at the tip of the laser probe 123.
  • the laser probe 123 is attached to the cavity 112 so that the tip thereof is desired in the internal space of the cavity 112.
  • the focal point of the condensing optical system 127 is located slightly below the lower opening of the cavity 112.
  • the laser light oscillated from the laser light source 121 passes through the condensing optical system 127 of the laser probe 123 and is condensed at the focal point of the condensing optical system 127.
  • the laser light source 21 for example, a microchip laser is used.
  • the condensing optical system 127 for example, a convex lens is used.
  • the output of the laser light source 121 is set so that the energy density of the laser light condensed at the focal point of the condensing optical system 127 is equal to or higher than the breakdown threshold of the analysis target substance 100. That is, the output of the laser light source 121 is set to be equal to or higher than a value necessary for the analysis target substance 100 present at the focal point to be turned into plasma.
  • the microwave oscillator 124 When the microwave oscillator 124 receives the microwave drive signal from the control device 114, the microwave oscillator 124 continuously outputs the microwave over the time of the pulse width of the electromagnetic wave drive signal.
  • the electromagnetic wave drive signal is a pulse signal having a constant voltage value.
  • the output of the microwave in the microwave oscillator 124 is set to an output value of 100 watts or less (for example, 80 watts) so that the powdery analyte 100 is not scattered.
  • the microwave oscillator 124 is connected to the antenna probe 126 via the microwave transmission line 125.
  • the antenna probe 126 is provided with a radiation antenna 128 for radiating microwaves that have passed through the microwave transmission line 125.
  • the antenna probe 126 is attached so that the distal end of the radiation antenna 128 faces the focal point of the condensing optical system 127.
  • the radiation antenna 128 is provided so that a strong electric field region by the microwave is formed including the focal point of the condensing optical system 127.
  • the microwave oscillator 124 outputs a microwave of 2.45 GHz.
  • the semiconductor oscillator generates microwaves.
  • a semiconductor oscillator that oscillates microwaves in other frequency bands may be used.
  • the optical analysis device 113 analyzes and analyzes plasma light emitted from the analyte 100 in the plasma state located in the plasma region P during the plasma maintenance period in which the plasma generation device 111 maintains the plasma by microwave energy.
  • Optical analysis means for analyzing the target substance 100 is configured.
  • the photoanalyzer 113 analyzes the analysis target substance 100 using a time integral value of the emission intensity of plasma light in an analysis period to be described later in the plasma maintenance period.
  • the optical analysis device 113 includes an optical probe 130, an optical fiber 131, a spectrometer 132, a photodetector 133, and a signal processing device 134.
  • the optical probe 130 is a device for deriving plasma light in the internal space of the cavity 112.
  • the optical probe 130 is obtained by attaching a lens capable of capturing a relatively wide range of light to the tip of a cylindrical casing.
  • the optical probe 130 is attached to the side surface of the cavity 112 so that plasma light emitted from the entire plasma region P can be introduced into the lens.
  • the spectroscope 132 is connected to the optical probe 130 via the optical fiber 131.
  • the spectroscope 132 takes in plasma light incident on the optical probe 130.
  • the spectroscope 132 uses a diffraction grating or a prism to disperse the incident plasma light in different directions depending on the wavelength.
  • a shutter for separating an analysis period for analyzing plasma light is provided at the entrance of the spectrometer 132.
  • the shutter is switched by the control device 114 between an open state in which light is allowed to enter the spectroscope 132 and a closed state in which light is not allowed to enter the spectroscope 132. If the exposure timing of the photodetector 133 can be controlled, the analysis period may be divided by controlling the photodetector 133.
  • the photodetector 133 is arranged to receive light in a predetermined wavelength band among the light dispersed by the spectroscope 132. In response to the command signal output from the control device 114, the photodetector 133 photoelectrically converts the received light in the wavelength band into an electrical signal for each wavelength and outputs the electrical signal.
  • a charge coupled device is used for the photodetector 133.
  • the electrical signal output from the photodetector 133 is input to the signal processing device 134.
  • the signal processing device 134 calculates a time integrated value of the emission intensity for each wavelength based on the electrical signal output from the photodetector 133.
  • the signal processing device 134 calculates a time integrated value (emission spectrum) of the emission intensity for each wavelength with respect to the plasma light incident on the spectrometer 132 during the analysis period in which the shutter is open.
  • the signal processing device 134 detects a wavelength component having a strong emission intensity from the time integrated value of the emission intensity for each wavelength, and identifies a substance corresponding to the detected wavelength component as a component of the analysis target substance 100. -Operation of the analyzer-
  • the analysis operation in which the analysis apparatus 10 performs component analysis of the analysis target substance 100 will be described.
  • the analysis operation is performed during the operation of the belt conveyor 101.
  • the plasma generation maintaining operation by the plasma generation device 111 and the optical analysis operation by the optical analysis device 113 are performed in conjunction with each other.
  • the plasma generation maintaining operation is an operation in which the plasma generating apparatus 111 generates and maintains plasma.
  • the plasma generation device 111 drives the laser light source 121 to generate an initial plasma according to an instruction from the control device 114, and drives the microwave oscillator 124 to irradiate the initial plasma with microwaves to maintain the plasma state. Perform maintenance operation.
  • the control device 114 outputs a laser oscillation signal (short pulse signal) to the laser light source 21.
  • the laser light source 121 oscillates only one pulsed laser beam.
  • the laser light oscillated from the laser light source 121 is condensed on the surface layer of the analyte 100 by the condensing optical system 127.
  • the analysis target substance 100 is momentarily given high-density energy.
  • the energy density of the laser light irradiation area increases and exceeds the breakdown threshold of the analysis target substance 100. If it does so, the substance of the irradiation area of a laser beam will ionize, and will be in a plasma state. That is, plasma (initial plasma) using the analysis target substance 100 as a raw material is generated.
  • the control device 114 outputs a microwave drive signal to the microwave oscillator 124 immediately after the fall of the laser oscillation signal.
  • the microwave oscillator 124 When receiving the microwave drive signal, the microwave oscillator 124 outputs a continuous wave (CW) of the microwave to the radiation antenna 128.
  • the microwave is radiated from the radiation antenna 128 to the internal space of the cavity 112.
  • the microwave is radiated from the radiating antenna 128 over the time of the pulse width of the microwave driving signal. Note that the time X from the falling point of the laser oscillation signal to the rising point of the electromagnetic wave drive signal is set so that microwave emission starts before the initial plasma disappears.
  • a region centered on the focal point of the condensing optical system 127 is a strong electric field region (a region where the electric field strength is relatively strong in the internal space of the cavity 112).
  • the initial plasma absorbs the microwave energy and expands to become a ball-shaped microwave plasma.
  • a plasma region P in which microwave plasma exists is formed so as to include the surface layer portion of the analysis target substance 100.
  • the microwave plasma is maintained over the microwave radiation period Y.
  • the microwave radiation period Y is a plasma maintenance period.
  • the microwave radiation period Y is, for example, several tens of microseconds to several tens of seconds. Even when the microwave oscillator 124 outputs microwaves for a relatively long time, the microwave output value is set to a predetermined value (for example, 80 watts) so that the microwave plasma does not become thermal plasma. Has been.
  • the time-series change in the emission intensity of the plasma light emitted from the plasma is first shown. Is seen instantaneously, and the emission intensity decreases to a minimum value close to zero. Then, after the emission intensity becomes a minimum value, there is an emission intensity increase period in which the emission intensity of the microwave plasma increases, and following the emission intensity increase period, the emission intensity is constant at which the microwave emission intensity becomes a substantially constant value. A period (period in which the amount of change (increase) in the emission intensity of the plasma light is a predetermined value or less) is observed.
  • the maximum value of the emission intensity of the plasma light during the plasma maintenance period is greater than the maximum value of the emission intensity of the plasma light before the microwave emission.
  • the microwave output during the plasma maintenance period is set so that is larger.
  • a large emission intensity can be obtained from the plasma light while preventing the analysis target substance 100 from being scattered, so that the analysis of the analysis target substance 100 can be performed more accurately.
  • the maximum value of the emission intensity of the plasma light before the microwave emission is higher than the emission intensity of the plasma light during the plasma maintenance period, as indicated by a broken line in FIG. You may set the microwave output of a plasma maintenance period so that it may become larger than the maximum value.
  • the optical analysis operation is an operation in which the optical analysis device 113 analyzes light (plasma light) emitted from the analysis target substance 100 in a plasma state.
  • the optical analysis device 113 performs an optical analysis operation for performing a spectral analysis of the plasma light and analyzing a component of the analysis target substance 100.
  • the analysis period is set within the fixed emission intensity period of the plasma maintenance period, and the analysis target substance is analyzed based on the emission intensity of the plasma light in the analysis period.
  • the control device 114 controls the shutter of the spectroscope so that the entire emission intensity stabilization period is set to the analysis period, and also controls the period during which the photodetector 133 performs photoelectric conversion. A part of the emission intensity stabilization period may be set as the analysis period.
  • the substance to be analyzed 100 is scattered by the shock wave generated by the laser beam.
  • the portion where the analysis target substance 100 is scattered passes through the plasma region P at the start of the period of constant emission intensity.
  • the analysis target substance 100 existing in the plasma region P at the start of the period in which the emission intensity is constant enters the plasma region P during the plasma maintenance period.
  • the analysis target substance 100 that has entered the plasma region P during the plasma maintenance period is not affected by scattering and is in a state where there is almost no movement of the substance.
  • plasma light emitted from the analysis target substance 100 in the plasma state located in the plasma region P passes through the optical probe 130 and the optical fiber 131 in order only during a certain period of emission intensity (analysis period) shown in FIG.
  • the light passes through and enters the spectroscope 132.
  • the incident plasma light is dispersed in different directions depending on the wavelength. Then, plasma light having a predetermined wavelength band reaches the photodetector 133. In the photodetector 133, the received plasma light in the wavelength band is photoelectrically converted into an electrical signal for each wavelength.
  • the signal processing device 134 calculates a time integrated value of the emission intensity for each wavelength for a fixed emission intensity period (analysis period). The signal processing device 134 creates a spectrum diagram showing the time integrated value of the emission intensity corresponding to the wavelength, as shown in FIG. The signal processing device 134 detects the wavelength at which the peak of the emission intensity appears from the time integrated value of the emission intensity for each wavelength, and identifies the substance (atom or molecule) corresponding to the detected wavelength as a component of the analysis target substance 100. .
  • the signal processing device 134 identifies molybdenum as a component of the analysis target substance 100 when a peak of emission intensity appears at 379.4 mm, for example. For example, when a peak of emission intensity appears at 422.7 mm, calcium is identified as a component of the analysis target substance 100. For example, when a peak of emission intensity appears at 345.2 mm, cobalt is identified as a component of the analysis target substance 100. For example, when a peak of emission intensity appears at 357.6 mm, chromium is identified as a component of the analysis target substance 100.
  • the spectrum diagram as shown in FIG. 4 may be displayed on the monitor of the signal processor 134 and the analyzer 10.
  • the user of the analyzer 10 can identify the components contained in the analysis target substance by looking at this spectrum diagram. -Effect of Embodiment 3-
  • the microwave energy is stably applied to the plasma region P during the plasma maintenance period, the generation of a shock wave due to the microwave is suppressed.
  • the analysis period in which the optical analyzer 113 performs analysis exists in the plasma maintenance period. Therefore, when the powdery substance is used as the analysis target substance 100, the analysis target substance 100 in the plasma region P can be prevented from being scattered during the analysis period. The analysis target substance 100 in the plasma region P can be analyzed with almost no movement of the substance.
  • powdery substances can be analyzed as they are.
  • the analysis target substance 100 when a powdery substance is used as the analysis target substance 100, the analysis is performed in a state of a pellet obtained by solidifying a powdery substance with a binder.
  • the powdery substance since the powdery substance can be analyzed as it is, the noise due to the binder does not appear in the light emission intensity, and the filter for removing the noise can be omitted.
  • the intensity of the microwave plasma during the plasma maintenance period is not so strong. Therefore, the metal which comprises the radiation antenna 128 is hardly excited, The noise resulting from such a metal can be suppressed.
  • the signal processing device 134 detects a mixing ratio of a plurality of components in the analysis target substance 100.
  • the plasma maintained by the plasma generation apparatus 111 of the third embodiment is larger than the plasma generated only by laser light. Therefore, by capturing plasma light in a large area, it becomes possible to detect the mixing ratio of components in that area.
  • the signal processor 134 stores calibration curve data indicating the relationship between emission intensity and content for a plurality of substances.
  • the signal processing device 134 detects a plurality of substances corresponding to the wavelength at which the emission intensity peak appears, and calculates the content of the detected substance based on the calibration curve data.
  • the signal processing device 134 calculates the ratio of the content of the substance corresponding to the wavelength at which the emission intensity peak appears, and detects the mixing ratio of the components contained in the analysis target substance.
  • the analyzer 10 when used for quality control of a medicine, it is possible to detect whether or not the mixing ratio of a specific component in the medicine is within a predetermined range.
  • the signal processing device 134 calculates the contents of the A component and the B component from the light emission intensities of the wavelengths corresponding to the A component and the B component included in the chemical powder, respectively.
  • the signal processing apparatus 134 calculates the mixing ratio (weight ratio of content) of B component with respect to A component from content of A component and content of B component.
  • the signal processing device 134 may correct the content of the substance obtained from the light emission intensity based on the energy of the reflected wave of the microwave in the radiation antenna 128 of the electromagnetic wave radiation device 116.
  • the larger the reflected wave the smaller the microwave energy input to maintain the microwave plasma and the lower the emission intensity.
  • the signal processing device 134 corrects the substance content calculated from the emission intensity to a larger value as the energy of the reflected wave of the microwave is larger.
  • the optical analyzer 113 analyzes the plasma light during the plasma maintenance period and detects the temperature of the gas in the microwave plasma region P.
  • Embodiment 4 The fourth embodiment is different from the third embodiment in the means for generating the initial plasma.
  • a spark plug 223 (discharger) is used to generate the initial plasma, as shown in FIG.
  • the controller 114 outputs a spark generation signal to the pulse voltage generator 121 when generating the initial plasma.
  • the pulse voltage generator 121 outputs a high voltage pulse to the spark plug 223, and a spark discharge is generated in the discharge gap between the electrodes 150 of the spark plug 223.
  • initial plasma is generated.
  • the high voltage pulse is an impulse voltage signal having a peak voltage of about 6 kV to 40 kV, for example.
  • the radiation antenna 128 is embedded in the spark plug 223.
  • the control device 114 outputs a microwave drive signal to the microwave oscillator 124 immediately after the fall of the spark generation signal.
  • the microwave oscillator 124 outputs a microwave from the radiation antenna 128 as a continuous wave.
  • the initial plasma generated by the spark discharge absorbs microwave energy and expands.
  • the radiation antenna 128 may be provided separately from the spark plug 223. ⁇ Other Embodiments >>
  • the above embodiment may be configured as follows.
  • the time integral value of the emission intensity used for the analysis of the analysis target substance 15 is the time integral value of the emission intensity only during the period in which the emission intensity by the microwave plasma is kept almost constant.
  • the integrated value of the emission intensity during the period in which the emission intensity is increased by the wave plasma may be included, or the emission intensity decreases after the microwave plasma is extinguished.
  • the integrated value of the emission intensity during the period to be included may be included.
  • the laser light source 21 may be a solid laser light source other than the Nd: YAG laser light source, or a liquid laser light source, a gas laser light source, a semiconductor laser light source, or a free electron laser light source. Also good.
  • the means for generating breakdown (initial plasma generating means) only needs to give sufficient energy to cause breakdown, and in addition to the laser light source 21 and the spark plug 54, It may be a thermionic generator such as a glow plug, a laser diode, or a high-intensity light emitting diode semiconductor light emitting element.
  • microwave oscillator 23 another oscillator such as a semiconductor oscillator may be used as the microwave oscillator 23.
  • the present invention is useful for an analysis apparatus and an analysis method for analyzing a substance to be analyzed by analyzing light emitted from plasma.
  • Analyzer plasma generating means
  • Plasma generator Cavity
  • Optical analyzer optical analysis means
  • Laser light source Condensing optical system
  • Microwave oscillator 28
  • Antenna 32
  • Optical element 33

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Abstract

L'invention concerne un dispositif d'analyse (10), pourvu d'un dispositif de génération de plasma (11) et d'un dispositif d'analyse photométrique (13). Le dispositif de génération de plasma (11) excite la matière dans l'air et génère un plasma initial, la matière étant à l'état de plasma, et maintient l'état de plasma en soumettant le plasma initial à des ondes électromagnétiques sur une durée prédéterminée. Le dispositif d'analyse photométrique (13) analyse la matière (15) à analyser à l'aide de l'intégrale temporelle de l'intensité d'émission de lumière émise par la matière (15) à analyser, dans la région du plasma maintenue par les ondes électromagnétiques.
PCT/JP2011/070774 2010-09-15 2011-09-12 Procédé et dispositif d'analyse WO2012036138A1 (fr)

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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2013039036A1 (fr) * 2011-09-12 2013-03-21 イマジニアリング株式会社 Analyseur et procédé d'analyse
JP2015530586A (ja) * 2012-09-27 2015-10-15 サントル ナショナル ドゥ ラ ルシェルシュ スィヤンティフィック（セーエヌエルエス）Ｃｅｎｔｒｅ Ｎａｔｉｏｎａｌ Ｄｅ Ｌａ Ｒｅｃｈｅｒｃｈｅ Ｓｃｉｅｎｔｉｆｉｑｕｅ（Ｃｎｒｓ） 低温プラズマ中の粒子を分析するための方法およびシステム
WO2015190617A1 (fr) * 2014-06-14 2015-12-17 イマジニアリング株式会社 Procédé d'analyse et dispositif d'analyse
JP2018504592A (ja) * 2014-12-31 2018-02-15 サーモ サイエンティフィック ポータブル アナリティカル インスツルメンツ インコーポレイテッド レーザ誘起ブレークダウン分光器の試料室
WO2018143355A1 (fr) * 2017-02-01 2018-08-09 イマジニアリング株式会社 Dispositif d'analyse

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001349832A (ja) * 2000-06-12 2001-12-21 Agency Of Ind Science & Technol レーザを用いた成分分析方法
JP3377699B2 (ja) * 1996-11-05 2003-02-17 三菱重工業株式会社 レーザを用いた微量成分計測手法及びその装置
JP2010025869A (ja) * 2008-07-23 2010-02-04 Imagineering Inc 物質分析装置

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3718672A1 (de) * 1987-06-04 1988-12-15 Metallgesellschaft Ag Verfahren zur analyse von metallteilchen
US6008897A (en) * 1999-01-19 1999-12-28 National Research Council Of Canada Method and apparatus for materials analysis by enhanced laser induced plasma spectroscopy
WO2008115287A2 (fr) * 2006-10-18 2008-09-25 Efthimion Enterprises, Inc. Spectroscopie au plasma micro-ondes assistée par laser
US7821634B2 (en) * 2007-04-20 2010-10-26 Thermo Niton Analyzers Llc Laser-triggered plasma apparatus for atomic emission spectroscopy

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3377699B2 (ja) * 1996-11-05 2003-02-17 三菱重工業株式会社 レーザを用いた微量成分計測手法及びその装置
JP2001349832A (ja) * 2000-06-12 2001-12-21 Agency Of Ind Science & Technol レーザを用いた成分分析方法
JP2010025869A (ja) * 2008-07-23 2010-02-04 Imagineering Inc 物質分析装置

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
See also references of EP2618132A4 *
SHOJI KANEKO ET AL.: "Micro-ha Assist Breakdown Bunkoho no Kenkyu", PREPRINTS OF MEETING ON AUTOMOTIVE ENGINEERS, 20 May 2009 (2009-05-20), pages 1 - 4, XP008169859 *

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2013039036A1 (fr) * 2011-09-12 2013-03-21 イマジニアリング株式会社 Analyseur et procédé d'analyse
US9606066B2 (en) 2011-09-12 2017-03-28 Imagineering, Inc. Analyzer and analysis method
JP2015530586A (ja) * 2012-09-27 2015-10-15 サントル ナショナル ドゥ ラ ルシェルシュ スィヤンティフィック（セーエヌエルエス）Ｃｅｎｔｒｅ Ｎａｔｉｏｎａｌ Ｄｅ Ｌａ Ｒｅｃｈｅｒｃｈｅ Ｓｃｉｅｎｔｉｆｉｑｕｅ（Ｃｎｒｓ） 低温プラズマ中の粒子を分析するための方法およびシステム
WO2015190617A1 (fr) * 2014-06-14 2015-12-17 イマジニアリング株式会社 Procédé d'analyse et dispositif d'analyse
JPWO2015190617A1 (ja) * 2014-06-14 2017-06-29 イマジニアリング株式会社 分析方法及び分析装置
JP2018504592A (ja) * 2014-12-31 2018-02-15 サーモ サイエンティフィック ポータブル アナリティカル インスツルメンツ インコーポレイテッド レーザ誘起ブレークダウン分光器の試料室
WO2018143355A1 (fr) * 2017-02-01 2018-08-09 イマジニアリング株式会社 Dispositif d'analyse

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JPWO2012036138A1 (ja) 2014-02-03
EP2618132A1 (fr) 2013-07-24
US20130208275A1 (en) 2013-08-15
US8879061B2 (en) 2014-11-04
JP5906501B2 (ja) 2016-04-20

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